Liquid State NMR Quantum Computing
... Obviously, this is true only so long as the coherent superposition states are preserved throughout the computation. This means that the computation should be completed before quantum coherence is lost due to “decoherence” processes (in NMR, spin–spin and spin-lattice relaxation; see Relaxation: An I ...
... Obviously, this is true only so long as the coherent superposition states are preserved throughout the computation. This means that the computation should be completed before quantum coherence is lost due to “decoherence” processes (in NMR, spin–spin and spin-lattice relaxation; see Relaxation: An I ...
Cabello`s nonlocality for generalized three
... product of the measurement outcomes of the observables X1 , Y2 , and Z3 . Indeed, both probability distributions (23) and (24) pertain to the only class of extremal two-way local correlations that are not fully local [15], which means that such correlations can be accounted for by a hybrid hidden va ...
... product of the measurement outcomes of the observables X1 , Y2 , and Z3 . Indeed, both probability distributions (23) and (24) pertain to the only class of extremal two-way local correlations that are not fully local [15], which means that such correlations can be accounted for by a hybrid hidden va ...
Detected-jump-error-correcting quantum codes - IAP TU
... quantum codes which are capable of stabilizing distinguishable qubits against spontaneous decay processes into statistically independent reservoirs 关12兴. These codes are constructed by embedding an active error-correcting code in a passive code space and by exploiting information available on error ...
... quantum codes which are capable of stabilizing distinguishable qubits against spontaneous decay processes into statistically independent reservoirs 关12兴. These codes are constructed by embedding an active error-correcting code in a passive code space and by exploiting information available on error ...
as a PDF
... classical version of this element is clearly not unitary. It doesn’t have as many outputs as inputs, so it can’t be reversible. It’s easy to see that even adding a third output isn’t enough to make the full adder reversible. The truth table for the classical full adder (see above) has 3 inputs which ...
... classical version of this element is clearly not unitary. It doesn’t have as many outputs as inputs, so it can’t be reversible. It’s easy to see that even adding a third output isn’t enough to make the full adder reversible. The truth table for the classical full adder (see above) has 3 inputs which ...
It is natural to think of quantum computations as multiparticle
... It is known that the dimensions of the physical system needed to encode a bit of information are becoming smaller and smaller, going towards the dimensions of a single atom. At atomic scale the laws of quantum mechanics govern the behaviour of physical systems. It turns out that quantum systems used ...
... It is known that the dimensions of the physical system needed to encode a bit of information are becoming smaller and smaller, going towards the dimensions of a single atom. At atomic scale the laws of quantum mechanics govern the behaviour of physical systems. It turns out that quantum systems used ...
Information Theory and Machine Learning
... When we wish to communicate with somebody we generally need to do so over an imperfect channel, be it a crackling telephone line, a noisy room or even just an unreliable internet connection. The channel will usually add noise to whatever we are saying/sending and so we need to protect against this. ...
... When we wish to communicate with somebody we generally need to do so over an imperfect channel, be it a crackling telephone line, a noisy room or even just an unreliable internet connection. The channel will usually add noise to whatever we are saying/sending and so we need to protect against this. ...
Entropy density of quasifree states supported by left/right movers
... (Nonvanishing density) Any strictly positive temperature in the system leads to a nonvanishing asymptotic entropy density. This is due to the fact, that, in such a case, the Toeplitz symbol ia has at least one eigenvalue with modulus strictly smaller than 1. (Strong subadditivity) The existence of a ...
... (Nonvanishing density) Any strictly positive temperature in the system leads to a nonvanishing asymptotic entropy density. This is due to the fact, that, in such a case, the Toeplitz symbol ia has at least one eigenvalue with modulus strictly smaller than 1. (Strong subadditivity) The existence of a ...
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... Likewise, a qubit is described by its quantum state. Two possible quantum states for a qubit correspond to the 0 and 1 of a classical bit. In quantum mechanics, however, any object that has two different states necessarily has a range of other possible states, called superpositions, which entail bot ...
... Likewise, a qubit is described by its quantum state. Two possible quantum states for a qubit correspond to the 0 and 1 of a classical bit. In quantum mechanics, however, any object that has two different states necessarily has a range of other possible states, called superpositions, which entail bot ...
Rewriting measurement-based quantum computations with
... The problem of producing a circuit equivalent to a given measurement-based quantum computation is of great importance. In [8], an automated translation has been proposed for measurement-based computations which have a causal flow. In [9], the author presents a similar technique based on causal flow ...
... The problem of producing a circuit equivalent to a given measurement-based quantum computation is of great importance. In [8], an automated translation has been proposed for measurement-based computations which have a causal flow. In [9], the author presents a similar technique based on causal flow ...
